BACKGROUND OF THE INVENTION
[0001] Microwave circuits are employed for coupling electromagnetic energy between microwave
components such as horns, circulators, signal generators and receivers. The conduits
by which the electromagnetic energy is coupled between the microwave components may
be constructed in various forms of transmission lines ranging from stripline to waveguide,
and frequently include various forms of power couplers, power splitters, and power
combiners. Such conduits allow microwave signals to be split among a number of microwave
components, and also allow the combining of signals from a plurality of microwave
components.
[0002] Of particular interest herein are complex microwave circuits employing coaxial transmission
lines, particularly rigid coaxial transmission lines having a center conductor of
rectangular or square cross section, for interconnecting numerous microwave components.
Such circuitry is found, by way of example, in large antenna arrays employing many
horn radiators coupled by signal combiners and/or splitters to produce a desired radiation
pattern. In such complex microwave structures, it is frequently necessary to bring
signals from various parts of the structure to other parts of the structure by coaxial
lines which cross over each other. An example of such routing of signals is found
in a matrix of interconnected signal paths such as a Butler matrix employed in converting
a signal input at one port of the matrix to a set of signals outputted by the matrix
for forming a beam. The crossings of signals in such matrix structures have been accomplished,
heretofore, by bending one transmission line about another.
[0003] A problem arises in that the complexity and size of a microwave structure is increased
by signal crossovers employing a bending of one coaxial transmission line about another.
It is recognized that a simplified form of such a structure is attained by placing
all components and connecting transmission lines in a single plane. However, a multiplicity
of crossovers comprising bent transmission lines can produce a considerable amount
of stacking of the transmission lines, one above the other. Such a mechanical configuration
is both bulky and heavy. Excessive bulk and weight are characteristics which are to
be avoided in the construction of antenna arrays, such as those employed in satellites,
wherein a reduction in space and weight is most desirable.
SUMMARY OF THE INVENTION
[0004] The foregoing problem is overcome and other advantages are provided by a coaxial
transmission-line crossover which, in accordance with the invention, can be constructed
without necessitating any increased height to the crossover structure as compared
to that of an individual coaxial line. This permits the microwave circuit to be constructed
in a planar microwave configuration.
[0005] In accordance with the invention, an in-plane configuration for a microwave crossover
is attained by connecting two hybrid couplers in tandem wherein each of the hybrid
couplers divides the power of an incoming electromagnetic wave into two waves of equal
power with a 90 degree phase shift between the two waves. Each of the hybrid couplers
has two input ports and two output ports, the output ports of a first one of the two
couplers being connected to the input ports of a second one of the two couplers.
[0006] The arrangement of the interconnection of the two couplers is accomplished by constructing
all conduits of electromagnetic power within a single planar configuration, in accordance
with a feature of the invention, by use of a coupler having two input ports on a front
side of the coupler and two output ports on a back side of the coupler. Such a coupler
is constructed by use of coaxial transmission lines connecting to the ports of the
coupler and wherein, within a housing of the coupler, diametrically opposed pairs
of input and output ports are connected by a pair of crossed insulated, electrically-conducting
rods or bars which are spaced apart by a uniform narrow gap to provide for capacitive
coupling of electromagnetic power between the two bars.
[0007] In accordance with yet another feature of the invention, an inplane configuration
for the crossing of the two bars is attained by the construction of a notch in a central
region of each bar, the notch of one bar facing the notch of the other bar at the
site of the crossover with one notch engaging with and enveloping the other notch
while maintaining a gap between the walls of the notch, through which gap there is
capacitive coupling of electromagnetic power. The effect of the crossover has the
effect of creating a half twist to the two bars, in a manner similar to a twisted
pair of electrical conductors, this resulting in a relocation of one input port and
one output port so as to place both input ports on the front side of the housing and
both output ports on the back side of the housing.
[0008] Two embodiments of the crossed configuration of the pair of bars within a metallic
housing are provided. In a first embodiment, each of the bars is provided with a pair
of end portions which extend transversely to the housing, the end portions being joined
by a central portion which is angled at approximately 45 degrees to offset the two
end portions and to provide opportunity for the crossing of one central portion over
the other central portion. The end portions of one bar are parallel to the corresponding
end portions of the other bar to provide for capacitive coupling of electromagnetic
power therebetween. A rectangularly shaped notch is provided in each of the central
portions of sufficient size to provide for a desired gap width between the central
portions in the crossover region for capacitive coupling of electromagnetic power
between the central portions, which capacitive coupling per unit of length of a bar
is substantially the same as the capacitive coupling per unit length of the bar at
the end portions, thereby to minimize any tendency to develop reflected waves at the
crossover. The overall length of the bars is approximately one-quarter wavelength
of the radiation, with the central portion being less than one-tenth of a wavelength
of the radiation.
[0009] In a second embodiment, both of the bars are replaced with bars having tapered extensions
beyond the foregoing end portions, the extensions being inclined throughout their
length, with a central portion parallel to the extensions and inclined to the two
end portions. The resulting zig-zag configuration allows opposed end portions of the
bars to be parallel to each other and to allow the crossing of one central portion
over the other central portion. The notches in the central portions have a generally
rectangular form with the end walls of the notches being stepped for increased bandwidth
of the coupler. In addition, sections of sidewalls of the bars which face each other
are angled relative to a central axis of the bar to establish a uniform gap width
between these sidewall sections for a predetermined amount of capacitive coupling
of electromagnetic radiation. In each bar, the central axis is parallel to each of
the end portions, the end portions being offset to opposite sides of the central axis,
while a narrow strip or isthmus of the central portion is parallel to and disposed
on the central axis. This configuration of the bars increases the bandwidth of the
coupler. Dielectric supports are positioned transversely of the housing on both sides
of the crossed central regions, and a positional dielectric spacer is placed within
each gap formed between opposed end portions on opposite sides of the engaging notches
of the central portions. In both embodiments, the bars have a rectangular or square
cross-sectional form.
BRIEF DESCRIPTION OF THE DRAWING
[0010] The aforementioned aspects and other features of the invention are explained in the
following description, taken in connection with the accompanying drawing wherein:
Fig. 1 is a plan view of the crossover of the invention formed within a planar configuration
of a metallic base plate with a cover plate shown partially cutaway to expose the
central conductors of coaxial transmission lines;
Fig. 2 is an end view of the crossover taken along the line 2-2 in Fig. 1;
Fig. 3 is an enlarged plan view of a fragmentary portion of one of two hybrid couplers
of the crossover of Fig. 1;
Figs. 4 and 5 show sectional views taken along lines 4-4 and 5-5, respectively, in
Fig. 3 to show details of bars in the crossover region of one of the couplers of the
crossover;
Fig. 6 is a view, similar to that of Fig. 3, showing an alternative embodiment of
the crossover region of a coupler;
Fig. 7 and 8 show, respectively, a plan view and a side view of a bar in the alternative
embodiment of the coupler of Fig. 6; and
Fig. 9 is a diagrammatic representation of the tandem arrangement of the two couplers
of Fig. 1 including paths of electromagnetic waves useful in explaining operation
of the crossover.
DETAILED DESCRIPTION
[0011] Figs. 1 and 2 show a crossover 20 formed of coaxial transmission lines 22 disposed
within a base plate 24 covered by a cover plate 26. In accordance with the invention,
the crossover 20 comprises two hybrid couplers 28 and 30 which are formed of crossed
sections of a center conductor 32 of coaxial lines 22. Fig. 2 shows a front end 34
of the crossover 20, the view of Fig. 2 showing a first input port 36, a second input
port 38, and the cover plate 26 disposed on top of the base plate 24. In Fig. 1, a
portion of the cover plate 26 is shown, and the balance of the view is shown sectioned
beneath the top surface of the base plate 24, as indicated in Fig. 2. The square cross
section of center conductors 32, as well as the the square cross section of the inner
surface of the outer conductor 40 of the transmission lines 22 are also shown in Fig.
2. It should be noted that, while the square cross sectional configuration of the
transmission lines 22 is employed in the preferred embodiment of the invention, the
teachings of the invention are applicable also to rectangular coaxial transmission
lines. Dielectric supports 42 position the center conductors 32 within the outer conductors
40 and insulate the center conductors from the outer conductors. To facilitate the
description in Fig. 1, only a few of the supports 42 are shown, it being understood
that such supports may be positioned in various locations along the transmission lines,
and may be given a well-known physical configuration which negates reflection of electromagnetic
waves.
[0012] Each of the hybrid couplers 28 and 30 provide for a splitting of an electromagnetic
wave into two waves of equal power, wherein the two waves differ in phase by 90 degrees.
As will be explained herein, each of the couplers 28 and 30 are fabricated in accordance
with a feature of the invention which provides that two input ports are located on
a front end of each of the couplers, and two output ports are located on the back
end of each of the couplers. By way of example, the two input ports 36 and 38 of the
crossover 20 also serve as input ports to the coupler 28. A similar pair of output
ports, namely, a first output port 44 and a second output port 46, are located at
the back end 48 of the crossover 20. The output ports 44 and 46 also serve as output
ports of the coupler 30. The couplers 28 and 30 are of identical construction.
[0013] As may be seen by the layout of the couplers 28 and 30 presented in Fig. 1, and by
the end view presented in Fig. 2, the coaxial transmission lines 22 are fabricated
in a convenient fashion by milling out channels 50 within the base plate 24 to provide
the outer conductors 40 of the transmission lines 22. The center conductors 32 are
then placed within the channels 50, and supported in their respective positions by
the supports 42. Thereupon, the assembly is completed by installing the cover plate
26 on top of the base plate 24. Both the base plate 24 and the cover plate 26, as
well as the center conductors 32, may be fabricated of an electrically conducting
material which is readily machined, such as aluminum.
[0014] As will be explained in further detail hereinafter with reference to Fig. 9, the
crossover 20 acts to couple an electromagnetic wave from one of the input ports to
the diagonally opposite output port, for example, from the second input port 38 to
the first output port 44. This is accomplished by virtue of the even splitting of
power at each of the couplers 28 and 30 with the phase lag of 90 degrees, this resulting
in a cancellation of waves at one of the output ports so that all of the power of
the input wave exits from the other output port.
[0015] It is noted that a particular feature of the invention is the construction of the
crossover 20 including all components of the couplers 28 and 30 and their interconnecting
transmission lines 22 within a single assembly of planar configuration. This is made
possible because of the presence of both input ports of a coupler on the front end
of the coupler, and the presence of both output ports on the back end of the coupler.
This arrangement of the ports of each of the couplers 28 and 30 allows for the interconnection
of the couplers via the transmission lines 22 as shown in the layout of Fig. 1, the
layout disclosing that all connections are accomplished within a common planar configuration
without the need for any transmission lines located outside of the assembly of Fig.
1. Both the plates 24 and 26 are of planar configuration and serve to form a housing
of planar configuration for the coupler 28 and for the coupler 30.
[0016] These novel features are a direct consequence of the novel construction of each of
the couplers 28 and 30, which construction will now be described in accordance with
the invention.
[0017] With reference to Figs. 1-5, the coupler 28 is formed with a central region 52 having
a crossover 54 of two center conductors 32. Since both of the couplers 28 and 30 have
identical construction, only the coupler 28 will be described in detail, it being
understood that the description of the coupler 28 applies equally well to the coupler
30. In the central region 52, each of the center conductors 32 takes the form of a
bar, there being two such bars 56 and 58 in the central region 52 and at the crossover
54. At the crossover 54, one bar crosses above the other bar which, by way of example,
is portrayed in Fig. 3 by a crossing of the bar 56 above the bar 58.
[0018] The crossover 54 is accomplished within the planar configuration by notching each
of the bars 56 and 58 with notches 60 which face each other and allow the bars 56
and 58 to pass through each other at the notches 60 within the confines of the thickness
of the bar 56 and the bar 58 as is shown in the side views of Figs. 4 and 5. The notches
60 are sufficiently large to provide for clearance between the bars 56 and 58 at the
crossover 54, the clearance maintaining electrical insulation between the two bars
56 and 58.
[0019] In Fig. 4, the bar 56 is shown to be notched at its bottom side, while Fig. 5 shows
that the bar 58 is notched at its top side. As shown in Figs. 1 and 3, the bars 56
and 58 are parallel to each other except at the crossover 54 where each of the bars
undergoes a 45 degree change in direction so as to cross the other bar at an angle
of 90 degrees. In each of the bars 56 and 58, the notch 60 is located at a crossing
strip 62, the crossing strip 62 introducing a reverse curve to the bar by virtue of
two turns of 45 degrees in opposite directions. The depth of each notch 60 is somewhat
greater than the thickness of the rod 56, 58 so as to provide clearance in the vertical
direction between the strips 62 of the two bars 56 and 58. Clearance is also provided
in the horizontal (parallel to the plane of the base plate 24) direction between a
strip 62 of one of the bars and the sides 64 of the notch 60 in the other of the two
bars.
[0020] The clearance between the two crossing strips 62 at the central portions of the bars
56 and 58, and clearance between parallel end portions of the bars 56 and 58 are selected
to produce a desired amount of capacitance for coupling electromagnetic power between
the bars 56 and 58. At an operating frequency in the range of 3.7 - 4.2 GHz (gigahertz)
wherein the free-space wavelength of the radiation has a nominal value of three inches,
the clearance between the parallel end portions of the bars 56 and 58 is selected
to define a gap 66 having a width of 30 mils. A larger clearance is provided at the
crossover 54 such that the spacing between the crossing strips 62 as well as between
a crossing strip 62 and sides 64 of a notch 66 are each equal to 50 mils. The larger
clearance at the crossover 54 reduces the capacitance to the crossover 54 so as to
equalize the amount of capacitance per unit length of the bar 56 or 58 throughout
the length of the bar including both the end portion and the region of the crossover
54. It is noted that, in the absence of such increased clearance at the crossover
54, the added length of gap along the sides 64 of a notch plus the bottom 68 of a
notch 60 tends to increase the amount of capacitance at the crossover 54. It is desired
to maintain uniform capacitance in the central region 52 of the coupler 28 so as to
minimize reflection of electromagnetic waves and insure a low value of VSWR (voltage
standing wave ratio). The foregoing increase of clearance at the crossover 54 produces
the desired reduction in the capacitance at the crossover 54 so as to equalize the
capacitance per unit length of bar.
[0021] In terms of operation of the coupler 28, the configuration of the crossed bars 56
and 58 in Fig. 3 has the form of a twisted pair of electrical conductors wherein only
one half twist is provided. Therefore, the two bars 56 and 58 may be viewed as a pair
of parallel bars through which electromagnetic power is coupled. The location of input
and output ports of the coupler 28 follows the twisting of the bars 56 and 58. In
addition, the implementation of the twist, as is provided by the crossover 54 maintains
electromagnetic coupling between the two bars 56 and 58 so that the desired amount
of coupled power is maintained, independently of the twisting of the bars 56 and 58.
Thereby, the coupler 28 can provide for a division of the electromagnetic power of
a wave incident upon the coupler 28 into two waves of equal power outputted from the
coupler 28 in substantially the same fashion as though the bars 56 and 58 were totally
straight. Thus, by construction of the crossover 54 to implement a twisting of the
bars 56 and 58, the effect in the operation of the coupler 28 is to interchange locations
of input and output ports, in accordance with the invention, such that the two output
ports are on the same side, namely the back side of the coupler 28 while the two input
ports also share a common side, namely the front side of the coupler 28. This provides
the coupler 28 with the requisite locations of input and output ports to allow the
arrangement of interconnection between the two couplers 28 and 30 in a planar configuration
as shown in Fig. 1.
[0022] It is also noted that, while the coupler 28 has been described for use with the crossover
20, the coupler 28 may also be employed in other microwave circuits for performing
algebraic combinations of electromagnetic signals. Since the coupler 28 is reciprocal
in its operation, it may be employed for both division of power in one wave among
two other waves, as well as for combining the power of two waves into one wave. Also,
the above noted gap width which has been established for a 3 dB coupling of power
can be enlarged to provide for a coupling of smaller amounts of power. In the preferred
embodiment of the invention, the following cross sectional dimensions of the transmission
lines 22 are employed; the center conductor 32 in cross section measures 0.2 inches
on a side, and the outer conductor 40 in cross section measures 0.5 inch on a side.
The length of the bars 56 and 58, as portrayed in Fig. 1, is one-quarter wavelength
of the electromagnetic energy propagating along the transmission lines 22. The width
W (Fig. 1) of a channel 50 is enlarged at the coupler 28 to provide room for both
of the center conductors 32, the width being increased by the width of one outer conductor
40. The form of electromagnetic wave propagating along a coaxial transmission line
22 is a TEM (transverse electromagnetic) wave. The impedance of a transmission line
22 is 50 ohms.
[0023] Fig. 6 shows a view of a hybrid coupler 70 which is an alternative embodiment of
the hybrid coupler 28 of Fig. 1. The coupler 70 is fabricated in the same way as the
coupler 28, and is formed of a base plate 72 in which channels 50 have been milled
out to form the outer conductors 40 of coaxial transmission lines 22, the lines 22
including a center conductor 32, as was disclosed in the construction of the hybrid
coupler 28 of Fig. 1. The view of Fig. 6 shows a layout of the components of the coupler
70 and has been formed by taking a section through the base plate 72 parallel to the
top surface thereof, as was done in the sectioning of the view of Fig. 1.
[0024] In the event that the coupler 70 is to be employed in the construction of a microwave
crossover circuit, such as the crossover 20 of Fig.1, then the base plate 72 would
be extended to include two of the couplers 70 with interconnecting transmission lines
22 in the same fashion as is disclosed for the construction of the crossover 20 of
Fig. 1. The configuration of the base plate 72, as shown in Fig. 6, suffices for the
creation of the two input ports 36 and 38, for each of the couplers 70 and the two
output ports 44 and 46 for each of the two couplers 70. These ports may be employed
for connection of the coupler 70 to various microwave circuits or components such
as another hybrid coupler. As was the case with the coupler 28, the input ports 36
and 38 of the coupler 70 are directed towards the front of the coupler, while the
output ports 44 and 46 of the couplers 70 are directed towards the back of the coupler.
The cross sectional dimensions of the center conductor 32 and the outer conductor
40 in each of the transmission lines 22 are the same as that disclosed for the coupler
28 of Fig. 1. It should be noted that the description of the construction of the coupler
70, as well as of the coupler 28, can also be employed for coaxial transmission lines
in which the center conductors have a nonrectangular cross-sectional shape such as
a circular or elliptical shape. However, the rectangular shape is preferred for 3
dB couplers wherein an input wave divides into two output waves of equal power.
[0025] The coupler 70 includes a central region 74 which differs from the central region
52 of the coupler 28 by the provision of a crossing strip 76 in each of two bars 78
and 80 which are narrower than the corresponding crossing strips 62 in the bars 56
and 58 of the coupler 28. The bars 78 and 80 of the coupler 70 (Fig. 6) correspond
respectively to the bars 56 and 58 of the coupler 28 (Figs. 1 and 3).
[0026] A further difference between the central region 74 and 52 is the provision in the
central region 74 of a notch 82 in each of the bars 78 and 80 which has a stepped
sidewall 84 (Figs. 7 and 8) instead of the straight side 64 (Figs. 3, 4, and 5) of
the notch 60. Yet a further distinction between the central regions 74 and 52 is the
inclusion at the edge of the central region 74 of a taper 86 (Figs. 6 and 7) on extension
or wing portions of the bars 78 and 80 approaching a crossover 88 (Fig. 6), such tapers
being absent in the coupler 28 of Fig, 1. The foregoing differences in structure between
the couplers 70 and 28 provide the coupler 70 with a better VSWR, and also increases
the operating bandwidth of the coupler 70 as compared to the coupler 28.
[0027] As may be seen by inspection of Figs. 6 and 1, the bars 78 and 80 have a more complex
structure than the bars 56 and 58. It should be noted that the two bars 78 and 80
have the same physical shape, the geometry of the bar 80, as portrayed in Fig. 6,
being obtained by turning the bar 78 upside down. Specific details in the construction
of the bar 78 and 80 may be obtained by reference to the detailed views of the bar
80 in Figs. 7 and 8. As the bar 80 extends inwardly from the extensions thereof, the
width of the bar 80 is reduced by the taper 86 to a value of approximately one-half
the original width such that the width of the crossing strip 76 is approximately 0.1
inch, as compared to 0.2 inches width at the ends of the bar 80. The crossing strip
76 is joined by necks 90 (Fig. 7) which are angled relative to the strip 76 so as
to offset both extensions of the bar 80 on opposite sides of a central axis 92 of
the bar 80. Both extensions of the bar 80, and the strip 76 are parallel to the axis
92, the strip 76 being centered on the axis 92. Inclination of a neck 90 relative
to an extension of the bar 80 is shown in Fig. 7 by an angle J equal to 135 degrees.
The inclination of both of the necks 90 to their respective bar extensions are the
same. Inclination of a taper 86 relative to a straight edge of an extension of the
bar 80 is shown in Fig. 7 by an angle H equal to 22.5 degrees. Both of the tapers
86 in the bar 80 have the same inclination.
[0028] The crossover 88 (Fig. 6) is similar to the crossover 54 (Figs. 1 and 3) in that,
in both cases, the crossing strip of one bar is enveloped by the notch of the the
other bar. As may be seen in Figs. 7 and 8, a bottom 94 of the notch 82 is sufficiently
wide to extend beyond the side edges of the crossing strip 76 in the crossover 88
(Fig. 6). Steps of the stepped sidewalls 84 extend still further back from the sides
of the crossing strip 76 in the crossover 88. Beyond the region of the crossover 88
and the necks 90, the bars 78 and 80 broaden to their initial width. Thus, the necks
90 and the crossing strip 76 can be viewed as an isthmus which joins the broader extensions
or wing portions of each of the bars 78 and 80.
[0029] As shown in Fig. 6, the bars 78 and 80 are held in position by means of two springs
96, two dielectric supports 98, and a pair of dielectric spacers 100. The springs
96 are secured within pockets 102 in a sidewall of a channel 50. The springs urge
the supports 98 towards each other and against the bars 78 and 80. The spacers 100
are oriented vertically with respect to the plane of the base plate 72 and are disposed
between facing sides of paired necks 90, there being one spacer 100 on opposite sides
of the crossover 88. The spacers 100 resist the forces exerted by the springs 96 as
the bars 78 and 80 are urged together, thereby tightly holding the bars 78 and 80
in their respective positions for maintaining a desired clearance between the necks
90 of the bars 78 and 80, and between the corresponding portions of the crossing strips
76 and the notches 82 at the crossover 88, As was the case with gaps and spacings
disclosed above with reference to the coupler 28, corresponding values are employed
in the coupler 70 of Fig. 6. Thus, the spacers 100 have a thickness of 30 mils, and
the vertical spacing between the bottom 94 of a notch 82 and the facing side of a
crossing strip 76 is 50 mils. With respect to the dimensions of the steps of the stepped
sidewall 84 (Fig. 8), the depth of the step is approximately one-third the depth of
the bottom 94 of the notch 82, while the horizontal portion of the step is approximately
one-third the width of the bottom 94.
[0030] An iris 104 (Fig. 6) is provided by two vanes 106 extending inwardly towards the
crossover 88 from outer sidewalls of channels 50, the vanes 106 being coplanar with
the spacers 100. The iris 104 serves to limit the region through which electromagnetic
power from an input port 36, 38 can couple to both of the output ports 44 and 46.
The length of the foregoing isthmus (the two necks 90 plus the crossing strip 76)
is one-quarter wavelength of the electromagnetic waves propagating along the transmission
lines 22, this length being less than the cross-sectional dimension of the iris 104.
In terms of the operation of the coupler 70, it is noted that the amount of power
coupled between the bars 78 and 80 depends on the capacitance between the two bars,
this being determined primarily by the coupling at the spacers 100 and at the crossover
88, while the difference in phase imparted between waves outputted at the ports 44
and 46 is determined by interaction of electromagnetic waves across the entire distance
of the iris 104. The material employed in the supports 98 and the spacers 100 is preferably
a plastic material having a dielectric constant of approximately 3.2, one such material
being marketed by General Electric under the trade name of ULTEM 1000, this material
being dimensionally stable, even at high temperatures.
[0031] Operation of the crossover 20 of Fig. 1 constructed with the hybrid couplers 28 and
30 is the same as the operation of the crossover 20 with two couplers 70 substituted
for the couplers 28 and 30. This operation is explained with the aid of the diagrammatic
representation of Fig. 9 which shows the two couplers 28 and 30 wherein output ports
of the coupler 28 are connected via transmission lines 22 to corresponding input ports
of the coupler 30. Also shown in Fig, 9 are the two input ports and the two output
ports of the crossover 20. In this explanation of the operation, it is presumed that
a wave enters the second input port at point G, and propagates along paths indicated
by dashed lines. Key points on the dashed lines are indicated at E and F in the coupler
28, and four waves resulting by operation of the couplers 28 and 30 appear at points
A, B, C, and D at the two output ports of the crossover 20.
[0032] In operation, the input wave at G splits at the coupler 28 into two waves E and F
having equal power, which power is equal to one-half of the original power at G. The
wave at E is shifted 90 degrees lagging relative to the wave at F. At the coupler
30, the wave E splits into two components B and C having equal power, the power in
the wave components B and C each being equal to one-quarter of the input power at
G. Similarly, the wave at F is split by the coupler 30 into two wave components A
and D having equal power, the power in each of the waves A and D being equal to one-quarter
of the power at G. The wave at C is shifted in phase by a lagging ninety degrees relative
to the wave at B. Similarly, the wave at A is shifted in phase by a lagging 90 degrees
relative to the wave at D. As a result of the phase shifting, the wave component at
C has undergone two ninety-degree phase shifts for a total phase shift of 180 degrees.
Therefore, the wave component C destructively interferes with the wave component D
resulting in a cancellation of all power outputted at the second output port. Therefore,
none of the power of the wave at E is coupled from the left side of the coupler 30
to the right side of the coupler 30; all of the power at E exits the first output
port. Similarly, none of the power at F exits the second output port, all of the power
being coupled from the right side of the coupler 30 to the left side of the coupler
30 to exit at the first output port. Since the coupling of power via the couplers
28 and 30 each introduce a lagging phase shift of 90 degrees, the contributions via
both couplers 28 and 30 are in phase at the first output port, the two contributions
at A and B each having a lagging phase shift of 90 degrees. Thus, the two contributions
at A and B add cophasally to produce an output power at the first output port equal
to the power inputted at the second input port. The wave outputted at the first output
port has a lagging phase of ninety degrees relative to the phase of the wave inputted
at the second input port.
[0033] It is to be understood that the above described embodiments of the invention are
illustrative only, and that modifications thereof may occur to those skilled in the
art. Accordingly, this invention is not to be regarded as limited to the embodiments
disclosed herein, but is to be limited only as defined by the appended claims.
1. A coupler for electromagnetic power, characterized by:
a housing of electrically conductive material having a top wall and a bottom wall,
there being a front wall, a back wall, a first sidewall and a second sidewall joining
said top wall to said bottom wall, said housing having four openings oriented normally
to a common plane, said top wall and said bottom wall being parallel to said common
plane, said openings being positioned serially around a center of said housing and
pointing outward in different directions;
center conductors (32) disposed in each of said openings to form therewith a first
input port and a second input port and a first output port and second output port,
said first input port and said first output port being located at opposite ends of
said first sidewall, said second input port and said second output port being located
at opposite ends of said second sidewall, said first input port and said second input
port being located at opposite ends of said front wall, and said first output port
and said second output port being located on opposite ends of said back wall; a pair
of bars (56, 58; 78, 80) electrically connecting ports of said first sidewall with
ports of said second sidewall, said bars (56, 58; 78, 80) being uniformly positioned
apart from each other and from an inner surface of said housing; and
means for twisting a first bar (56; 78) of said pair of bars (56, 58; 78, 80) about
a second bar (58; 80) of said pair of bars (56, 58; 78, 80) with a half twist to enable
said first bar (56; 78) to interconnect said first input port with said second output
port, and to enable said second bar (58; 80) to interconnect said second input port
with said first output port.
2. The coupler of claim 1, characterized in that each of said bars (56, 58; 78, 80)
has a central portion, and a first end portion and a second end portion joined by
said central portion, said first end portion and said second end portion being straight
and of equal length, said twisting means comprising the central portions of said first
and second bars (56, 58; 78, 80).
3. The coupler of any of claims 1 or 2, characterized in that each of said bars (56,
58; 78, 80) has a rectangular cross-section and flat outer surfaces, one of said flat
surfaces being planar throughout the length of the said bar (56, 58; 78, 80), the
sum of the lengths of the two end portions plus the central portion in each of said
bars (56, 58; 78, 80) being approximately one-quarter wavelength of radiation propagating
through said couplers (28, 30; 70).
4. The coupler of claim 3, characterized in that said one planar surface of one of
said bars (56; 78) is parallel to said one planar surface of the other of said bars
(58; 80), said half twist retaining the planar configuration of said one planar surface
in each of said bars (56, 58; 78, 80).
5. The coupler of any of claims 1 through 4, characterized in that said twisting
means comprises the central portion of said first and second bars (56, 58; 78, 80),
in each of said bars (56, 58; 78, 80) said central portions having a notch (60, 66;
82) opposite said one planar surface, the notch (60) of said first bar (56) facing
and interleaving the notch (66) of said second bar (58).
6. The coupler of any of claims 1 through 5, characterized in that end portions of
each bar (56, 58; 78, 80) are parallel to the front wall and the back wall of said
housing.
7. The coupler of any of claims 1 through 6, characterized in that in each bar (56,
58; 78, 80), said central portion is angled relative to first and second end portions
of the bar (56, 58; 78, 80) to permit an interleaving and crossing configuration of
the central portions of said first and second bars (56, 58; 78, 80) of a coupler (28,
30,;70).
8. The coupler of any of claims 1 through 7, characterized in that there is capacitance
between said first bar (56; 78) and said second bar (58; 80) for coupling an electromagnetic
wave between said first bar (56; 78) and said second bar (58; 80), the capacitance
per unit length of an end portion of a bar (56, 58; 78, 80) being established by a
clearance between end portions of said first and said second bars (56, 58; 78, 80),
and that the clearance between central portions of said bars (56, 58; 78, 80) in the
notches (60, 66; 82) of said central portions is enlarged relative to the clearance
between said end portions of said bars (56, 58; 78, 80) to provide for a capacitance
per unit length of said central portions of said bars (56, 58; 78, 80) substantially
equal to the capacitance per unit length of the end portions of said bars (56, 58;
78, 80), thereby to inhibit the formation of reflected waves of electromagnetic power.
9. The coupler of any of claims 1 through 8, characterized in that each bar (78,
80) has a first and a second extension beyond said first and second end portions,
respectively, the central portion being parallel to a central longitudinal axis (92),
the two extensions of the bar (78, 80) being parallel to and offset to opposite sides
of said axis (92), the axes (92) of the two bars (78, 80) being angled to provide
for a crossover (88) of the central portions of each of said bars (78, 80).
10. The coupler of any of claims 1 through 9, characterized in that in each bar (56,
58; 78, 80), said one planar surface is parallel to said bottom wall, and each bar
(56, 58; 78, 80) has opposing sidewalls intersecting said one planar surface, sections
(64; 84) of the sidewalls on opposite sides of the central portion in said first bar
(56; 78) facing corresponding sidewall sections (64; 84) of said second bar (58; 80)
being angled relative to said central axis of said first bar (56; 78).
11. The coupler of any of claims 1 through 10, characterized in that corresponding
sidewall sections of the extensions of said second bar (80) are angled to the central
axis (92) of said second bar (80) equally with a corresponding sidewall section angulation
of the extensions of said first bar (78), the sum of angulations of the sidewall sections
of said first and second second bars (78, 80) being equal to approximately half a
crossing angle of axes (92) of said first and said second bars (78, 80), thereby to
provide a taper (86) to said extensions of said bars (78, 80).
12. The coupler of any of claims 5 through 11, characterized in that each notch (82)
is a double stepped notch (82, 84, 94).
13. The coupler of any of claims 11 or 12, characterized in that in each bar (78,
80) the central portion is narrowed relative to the extensions of the bar (78, 80)
by angulation of the sidewall sections relative to the central axis (92), the narrowing
of the central portion producing an isthmus of smaller cross-section than said extensions.
14. The coupler of any of claims 1 through 13, characterized in that said housing
includes an iris (104) comprising vanes (106) extending from sidewalls of the housing
between the end portions of said first and said second bars (78, 80).
15. The coupler of any of claims 5 through 14, characterized by a dielectric spacer
(100) disposed between opposed end portions on opposite sides of a gap formed by the
notches (82) of said first and said second bars (78, 80).
16. The coupler of any of claims 1 through 15, characterized by a front dielectric
support (42; 98) disposed between said front wall and end portions of each of said
bars (56, 58; 78, 80) and a back dielectric support (42; 98) disposed between said
back wall and end portions of each of said bars (56, 58; 78, 80).
17. The coupler of any of claims 5 through 16, characterized in that the length of
each of said notches (60, 66; 82) is less than one-tenth of the wavelength of an electromagnetic
wave propagating through the coupler (28, 30; 70).
18. The coupler of any of claims 5 through 17, characterized in that said notches
(60, 66; 82) of the central portion of each of said bars (56, 58; 78, 80) envelope
each other to a sufficient depth to provide for an in-plane crossing of an electromagnetic
wave propagating through the coupler (28, 30; 70).
19. The coupler of any of claims 1 through 18, characterized by means for supporting
each of said bars (56, 58; 78, 80) within said housing and insulated from each other
and from said housing.
20. The coupler of any of claims 1 through 19, characterized in that an extension
of said first bar (56; 78) is angled relative to the opposed extension of said second
bar (58; 80) by an angle of 90 degrees.
21. The coupler of any of claims 1 through 20, being a first hybrid coupler (28) and
being connected to a second hybrid coupler (30) of any of claims 1 through 20 to thereby
establish a coaxial transmission-line crossing element, characterized by:
said first hybrid coupler (28) and said second hybrid coupler (30), each of said couplers
(28, 30) having a first input port, a second input port, a first output port, and
a second output port; and wherein said first output port of said first coupler (28)
is connected to said first input port of said second coupler (30), said second output
port of said first coupler (28) is connected to said second input port of said second
coupler (30), said first and said second input ports of said first coupler (28) serving
as input ports (36, 38) of said crossing element, and said first and said second output
ports of said second coupler (30) serving as output ports (44, 46) of said crossing
element.